Heavy Quarkonium Properties at Finite Temperature in Strongly Coupled Quark Gluon Plasma

Rethika, K. T.; Ravikumar, C.; Bannur, Vishnu M.

doi:10.1007/s00601-021-01592-6

Cited by 4 publications

(1 citation statement)

References 25 publications

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“…The calculation of the EOS are based on the parameters of the temperature T and the chemical potential µ of the phenomenologically created matter of free quarks and gluons [13]. And the study in this regard from heavy quarks has been found in some of the literature also [14] Therefore, we expect a sharp transition from a confined hadronic phase to a deconfined phase of non-interacting colored quarks and gluons. In order to study about these phase transition structure of QCD we consider the entangled PNJL model with a Polyakov loop scale parameter that depends on the magnetic field.…”

Section: Introductionmentioning

confidence: 98%

Thermodynamic equation of state of magnetized PNJL model of 2 + 1 flavor at finite baryonic density

SINGH

2023

Preprint

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We extend our recent research work for 2 flavor magnetized PNJL model to 2 + 1 flavor quarkscooperating the finite baryonic potential in the thermal mass and magnetic field in the potential ofthe Lagrangian density. The evaluation of equation of state (EOS) and its relevant thermodynamicproperties after incorporating the finite chemical potential in the thermal mass and magnetic field inthe potential are represented in the results. The results show that all the thermodynamic parametersare found improved by the inclusion of the finite baryonic chemical potential. The result at the finitebaryonic density also conforms and improves from our earlier work without the baryonic chemicalvalue. It means there is an up-gradation in the outputs predicted by the presence of baryonic chemical potential in the thermal mass.

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Section: Introductionmentioning

confidence: 98%

Thermodynamic equation of state of magnetized PNJL model of 2 + 1 flavor at finite baryonic density

SINGH

2023

Preprint

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Properties of b$${\overline{c}}$$ and c$${\overline{s}}$$ mesons at finite temperature in strongly coupled quark gluon plasma

2022

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Thermodynamic properties of heavy mesons in strongly coupled quark gluon plasma using the fractional of non-relativistic quark model

Abu‐Shady

Ezz-Alarab

2023

Indian J Phys

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A generalized fractional derivative of the analytical exact iteration method is used, in which the two-body potential in strongly coupled quark–gluon plasma is devoted to solve the N-dimensional radial Schrödinger equation. The energy eigenvalues for any state (n, l) and mass spectra in the N-dimensional space have been investigated. The dissociation temperatures were computed in the N-dimensional space for different states of quarkonia. The effect of fractional-order parameter is investigated on the dissociation temperatures of heavy quarkonium masses such as charmonium and bottomonium and thermodynamic properties such as entropy, free energy, internal energy, and specific heat in the 3D and the higher-dimensional space. Also, the effect of dimensionality number on dissociation temperatures is discussed. A comparison with other recent works is displayed. We deduce that the fractional-order plays an essential role in 3D and higher-dimensional space.

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Heavy Quarkonium Properties at Finite Temperature in Strongly Coupled Quark Gluon Plasma

Cited by 4 publications

References 25 publications

Thermodynamic equation of state of magnetized PNJL model of 2 + 1 flavor at finite baryonic density

Thermodynamic equation of state of magnetized PNJL model of 2 + 1 flavor at finite baryonic density

Properties of b$${\overline{c}}$$ and c$${\overline{s}}$$ mesons at finite temperature in strongly coupled quark gluon plasma

Thermodynamic properties of heavy mesons in strongly coupled quark gluon plasma using the fractional of non-relativistic quark model

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